respectively.
Using [1]}, it immediately follows that there exists a bulk stretching strain \(e:\Omega -\lbrace S\cup \lbrace O\rbrace \rbrace \rightarrow \operatorname{Sym}\) , satisfying \(E(\psi )=\int _\Omega \left\langle e,\psi  \right\rangle \operatorname{da}\)  for all \(\psi  \in \mathcal {D}(\Omega -O,\operatorname{Lin})\) , and a bulk bending strain \(\lambda :\Omega -\lbrace S\cup \lbrace O\rbrace \rbrace \rightarrow \operatorname{Sym}\)  and a concentrated (on \(S\) ) bending strain \(\gamma  : S-\lbrace O\rbrace \rightarrow \operatorname{Sym}\) , satisfying \(\Lambda (\psi )=\int _\Omega \left\langle \lambda ,\psi  \right\rangle \operatorname{da}+ \int _S\left\langle \gamma ,\psi  \right\rangle \operatorname{dl}\)  for all \(\psi  \in \mathcal {D}(\Omega -O,\operatorname{Lin})\) ,
such that
\(e = \frac{1}{2}\left( \nabla u +\nabla u^T \right) + \nabla w \otimes \nabla w ~\text{in}~ \Omega -\lbrace S\cup \lbrace O\rbrace \rbrace ,\\\lambda  = \nabla \nabla w ~\text{in}~ \Omega -\lbrace S\cup \lbrace O\rbrace \rbrace ,~\text{and}\\\gamma  = - \llbracket \nabla w \rrbracket \otimes \nu  ~\text{on}~ S-\lbrace O\rbrace .\) 
